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JPH089670B2 - Polyester film - Google Patents
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JPH089670B2 - Polyester film - Google Patents

Polyester film

Info

Publication number
JPH089670B2
JPH089670B2 JP62054584A JP5458487A JPH089670B2 JP H089670 B2 JPH089670 B2 JP H089670B2 JP 62054584 A JP62054584 A JP 62054584A JP 5458487 A JP5458487 A JP 5458487A JP H089670 B2 JPH089670 B2 JP H089670B2
Authority
JP
Japan
Prior art keywords
film
present
inorganic particles
width
polyester
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP62054584A
Other languages
Japanese (ja)
Other versions
JPS63221136A (en
Inventor
晃一 阿部
聡 西野
秀真 岡阪
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toray Industries Inc
Original Assignee
Toray Industries Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toray Industries Inc filed Critical Toray Industries Inc
Priority to JP62054584A priority Critical patent/JPH089670B2/en
Publication of JPS63221136A publication Critical patent/JPS63221136A/en
Publication of JPH089670B2 publication Critical patent/JPH089670B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03CPHOTOSENSITIVE MATERIALS FOR PHOTOGRAPHIC PURPOSES; PHOTOGRAPHIC PROCESSES, e.g. CINE, X-RAY, COLOUR, STEREO-PHOTOGRAPHIC PROCESSES; AUXILIARY PROCESSES IN PHOTOGRAPHY
    • G03C1/00Photosensitive materials
    • G03C1/76Photosensitive materials characterised by the base or auxiliary layers
    • G03C1/795Photosensitive materials characterised by the base or auxiliary layers the base being of macromolecular substances
    • G03C1/7954Polyesters

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Materials Engineering (AREA)
  • General Physics & Mathematics (AREA)
  • Manufacture Of Macromolecular Shaped Articles (AREA)
  • Shaping By String And By Release Of Stress In Plastics And The Like (AREA)
  • Compositions Of Macromolecular Compounds (AREA)
  • Magnetic Record Carriers (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は二軸配向ポリエステルフィルムに関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention relates to a biaxially oriented polyester film.

[従来の技術] 二軸配向ポリエステルフィルムとしては、ポリエステ
ルに不活性無機粒子を含有せしめたフィルムが知られて
いる(例えば、特開昭59−178224号公報)。
[Prior Art] As a biaxially oriented polyester film, a film made of polyester containing inert inorganic particles is known (for example, JP-A-59-178224).

[発明が解決しようとする問題点] しかし、上記従来の二軸配向ポリエステルフィルム
は、フィルムの加工工程、例えば包装用途における印刷
工程、磁気媒体用途における磁性層塗布、・カレンダー
工程などの工程速度の増大にともない接触するロールな
どでフィルムの表面が削れることにより、加工工程上、
製品性能上のトラブルとなるという欠点が最近問題とな
ってきている。
[Problems to be Solved by the Invention] However, the above-mentioned conventional biaxially oriented polyester film has a process speed of a film processing step, for example, a printing step in a packaging application, a magnetic layer application in a magnetic medium application, and a calendar step. As the surface of the film is scraped with a roll that comes into contact with the increase,
Recently, the drawback of product performance has become a problem.

本発明はかかる問題点を改善し、表面の「耐削れ性」
の優れたフィルムを提供することを目的とする。
The present invention solves these problems and improves the surface "scratch resistance".
It is intended to provide an excellent film of.

[問題点を解決するための手段] ポリエステルと、少なくとも一種類の不活性無機粒子
からなる組成物を主たる成分とする二軸配向フィルムで
あって、少なくとも片面のフィルムの極表層のカルボニ
ル基によるラマンバンドの半価幅が、フィルム内部の半
価幅より1cm-1以上大きいことを特徴とする二軸配向ポ
リエステルフィルムとしたものである。
[Means for Solving Problems] A biaxially oriented film containing a polyester and a composition comprising at least one kind of inert inorganic particles as a main component, wherein Raman by a carbonyl group of the polar surface layer of at least one surface of the film is used. The biaxially oriented polyester film is characterized in that the full width at half maximum of the band is 1 cm -1 or more larger than the full width at half maximum inside the film.

本発明におけるポリエステルとは、エチレンテレフタ
レート、エチレンα,β−ビス(2−クロルフェノキ
シ)エタン−4,4′−ジカルボキシレート、エチレン2,6
−ナフタレート単位から選ばれた少なくとも一種の構造
単位を主要構成成分とする。ただし、本発明を阻害しな
い範囲内、好ましくは5モル%以内であれば他成分が共
重合されていてもよい。
The polyester in the present invention means ethylene terephthalate, ethylene α, β-bis (2-chlorophenoxy) ethane-4,4′-dicarboxylate, ethylene 2,6
-At least one structural unit selected from naphthalate units is the main constituent. However, other components may be copolymerized within a range not hindering the present invention, preferably within 5 mol%.

また、エチレンテレフタレートを主要構成成分とする
ポリエステルの場合に耐削れ性がより一層良好となるの
で特に望ましい。
Further, in the case of polyester having ethylene terephthalate as a main constituent component, abrasion resistance is further improved, which is particularly desirable.

本発明における不活性無機粒子の種類は特に限定され
ないが、その結晶化促進係数が−5〜20℃、好ましくは
−5〜15℃、さらに好ましくは0〜10℃の範囲である場
合に、本発明範囲のラマンバンド半価幅が極めて得られ
やすくなるので特に望ましい。更にその中でも、コロイ
ド状シリカに起因する実質的に球形のシリカ、合成炭酸
カルシウム、酸化チタン、α−アルミナが特に望まし
い。ここでいうコロイド状シリカとはケイ酸ナトリウム
を原料とし、アルカリ分を除去してゆく過程で生成した
粒子であるのが望ましい。
The type of the inert inorganic particles in the present invention is not particularly limited, but when the crystallization acceleration coefficient is in the range of -5 to 20 ° C, preferably -5 to 15 ° C, more preferably 0 to 10 ° C, The Raman band full width at half maximum in the range of the invention is very easily obtained, which is particularly desirable. Furthermore, among them, substantially spherical silica derived from colloidal silica, synthetic calcium carbonate, titanium oxide, and α-alumina are particularly desirable. The colloidal silica referred to here is preferably particles produced from sodium silicate as a raw material in the process of removing alkali components.

本発明における不活性無機粒子の含有量は特に限定さ
れないが、0.05〜1.0重量%、特に0.1〜0.8重量%であ
る場合に耐削れ性がより一層良好となるので特に望まし
い。
The content of the inert inorganic particles in the present invention is not particularly limited, but is preferably 0.05 to 1.0% by weight, particularly 0.1 to 0.8% by weight because the abrasion resistance is further improved.

本発明における不活性無機粒子の平均粒径は特に限定
されないが、0.1〜1.0μm、特に0.15〜0.8μmである
場合に耐削れ性がより一層良好となるので特に望まし
い。
The average particle size of the inert inorganic particles in the present invention is not particularly limited, but is preferably 0.1 to 1.0 μm, particularly 0.15 to 0.8 μm because the abrasion resistance is further improved.

本発明における不活性無機粒子は2種類以上でもよい
し、また、同種類で平均粒径の異なる2種類以上のもの
を組合せて用いても内部析出粒子と併用してもよい。本
発明フィルムは、上記組成物を主要成分とするが、本発
明の目的を阻害しない範囲内で、他種ポリマをブレンド
してもよいし、また酸化防止剤、熱安定剤、滑剤、紫外
線吸収剤、核生成剤などの無機または有機添加剤が通常
添加される程度添加されていてもよい。
The inert inorganic particles in the present invention may be two or more kinds, or two or more kinds of the same kind having different average particle diameters may be used in combination or may be used in combination with the internally precipitated particles. The film of the present invention contains the above-mentioned composition as a main component, but may be blended with other polymers within a range that does not impair the object of the present invention, and may further contain an antioxidant, a heat stabilizer, a lubricant, and an ultraviolet absorbing agent. Inorganic or organic additives such as agents and nucleating agents may be added to the extent that they are usually added.

本発明フィルムは上記組成物を二軸配向せしめたフィ
ルムである。未延伸フィルム、一軸配向フィルムでは耐
削れ性が不良となるので好ましくない。
The film of the present invention is a film in which the above composition is biaxially oriented. An unstretched film or a uniaxially oriented film is not preferable because it has poor abrasion resistance.

また、その二軸配向の程度を表わす面配向指数は特に
限定されないが、0.935〜0.975、特に0.940〜0.970の範
囲である場合に、耐削れ性がより一層良好となるので特
に望ましい。
Further, the plane orientation index showing the degree of the biaxial orientation is not particularly limited, but it is particularly desirable in the range of 0.935 to 0.975, particularly 0.940 to 0.970 because the abrasion resistance is further improved.

本発明フィルムのフィルム極表層のカルボニル基の伸
縮振動に基づくラマンバンドの半価幅は、フィルム内部
のカルボニル基の伸縮振動に基づくラマンバンドの半価
幅よりも1cm-1、好ましくは2cm-1以上大きいことが必要
である。これらの半価幅の差が上記の範囲より小さい
と、フィルムの耐削れ性が不良となるので好ましくな
い。なお、この差の上限は特に限定されないが、通常8c
m-1程度が製造上の限界である。ここで、上記の半価幅
は後述の方法で測定されるものであるが、カルボニル基
の伸縮振動に基づくラマンバンドの半価幅はポリエステ
ルの密度と反比例の関係があることは、A.J.Melvegerに
よって報告されているものである(J.Polymer Science
10,317,1972)。
The half width of the Raman band based on the stretching vibration of the carbonyl group of the film electrode surface layer of the film of the present invention is 1 cm -1 than the half width of the Raman band based on the stretching vibration of the carbonyl group inside the film, preferably 2 cm -1. More than that is necessary. If the difference between these half widths is smaller than the above range, the abrasion resistance of the film becomes poor, which is not preferable. The upper limit of this difference is not particularly limited, but is usually 8c.
The manufacturing limit is about m -1 . Here, the above-mentioned full width at half maximum is to be measured by the method described below, but the full width at half maximum of the Raman band based on stretching vibration of the carbonyl group is inversely related to the density of the polyester, reported by AJ Melveger. (J. Polymer Science
10 , 317,1972).

また、本発明フィルムの極表層のカルボニル基のラマ
ンバンドの半価幅は特に限定されないが、15cm-1以上、
好ましくは17cm-1以上である場合に、耐削れ性がより一
層良好となるので特に望ましい。
Further, the full width at half maximum of the Raman band of the carbonyl group of the extreme surface layer of the film of the present invention is not particularly limited, 15 cm -1 or more,
When it is preferably 17 cm -1 or more, the abrasion resistance is further improved, which is particularly desirable.

本発明フィルムは、幅方向の表面平均粗さRaが0.005
〜0.030μm、特に0.007〜0.020μmの範囲である場合
に、耐削れ性がより一層良好となるので特に望ましい。
The film of the present invention has a surface average roughness Ra in the width direction of 0.005.
˜0.030 μm, particularly 0.007 to 0.020 μm, it is particularly desirable because the abrasion resistance is further improved.

本発明フィルムは、290℃、200sec-1で溶融粘度が100
0〜10000ポイズ、特に2000〜7000ポイズの範囲である場
合に、耐削れ性がより一層良好となるので特に望まし
い。
The film of the present invention has a melt viscosity of 100 at 290 ° C. and 200 sec −1.
A range of 0 to 10000 poises, particularly 2000 to 7000 poises, is particularly desirable because the abrasion resistance is further improved.

次に本発明フィルムの製造方法について説明する。 Next, a method for producing the film of the present invention will be described.

まず、所定のポリエステルに不活性無機粒子を含有せ
しめる方法としては、重合前重合中、重合後のいずれに
添加してもよいが、ポリエステルのジオール成分である
エチレングリコールに、スラリーの形で混合、分散せし
めて添加する方法が本発明の関係式を満足させるのに有
効である。また、不活性無機粒子の含有量を調節する方
法としては、高濃度のマスターペレットを製膜時に希釈
する方法が本発明範囲のラマンバンド半価幅を得るのに
有効である。この場合、モース硬度が3以上の不活性無
機粒子を用いて、エチレングリコール分散時に、195℃
で2時間熱処理する方法、あるいは無機粒子に対し0.5
〜20重量%のリン酸アンモニウム塩を添加する方法がフ
ィルム極表層および内部のラマンバンド半価幅の関係を
本発明範囲とするのに極めて有効である。
First, as a method of incorporating inert inorganic particles into a predetermined polyester, it may be added during polymerization before polymerization or after polymerization, but it is mixed with ethylene glycol, which is a diol component of polyester, in the form of a slurry, The method of adding after dispersion is effective for satisfying the relational expression of the present invention. Further, as a method of adjusting the content of the inert inorganic particles, a method of diluting a high-concentration master pellet during film formation is effective in obtaining the Raman band half width within the range of the present invention. In this case, by using inert inorganic particles having a Mohs hardness of 3 or more, 195 ° C at the time of ethylene glycol dispersion.
Heat treatment for 2 hours, or 0.5 for inorganic particles
The method of adding about 20% by weight of ammonium phosphate salt is extremely effective in controlling the relationship between the half-width of Raman band in the surface layer of the film and the inner half of the Raman band.

かくして、所定量の不活性無機粒子を含有するペレッ
トを十分乾燥したのち、公知の溶融押出機に供給し、27
0〜330℃でスリット状のダイからシート状に押出し、キ
ャスティングロール上で冷却固化せしめて未延伸フィル
ムを作る。この場合、押出時のドラフト比(口金スリッ
ト間隙/未延伸フィルム厚さ)を5〜30、好ましくは8
〜20の範囲にすることが本発明のラマンバンド半価幅を
満足させるのに有効である。
Thus, after sufficiently drying the pellets containing a predetermined amount of inert inorganic particles, it is supplied to a known melt extruder, 27
It is extruded into a sheet from a slit die at 0 to 330 ° C., and cooled and solidified on a casting roll to prepare an unstretched film. In this case, the draft ratio at the time of extrusion (die slit gap / unstretched film thickness) is 5 to 30, preferably 8
It is effective to set the range of -20 to satisfy the Raman band half width of the present invention.

次にこの未延伸フィルムを二軸延伸し、二軸配向せし
める。延伸方法としては、逐次二軸延伸法または同時二
軸延伸法を用いることができる。
Next, this unstretched film is biaxially stretched and biaxially oriented. As a stretching method, a sequential biaxial stretching method or a simultaneous biaxial stretching method can be used.

逐次二軸延伸法の場合は長手方向、幅方向の順に延伸
するのが一般的であるが、この順を逆にして延伸しても
よい。二軸延伸の条件は延伸方法、ポリマの種類などに
よって必ずしも一定ではないが、通常、長手方向、幅方
向ともに80〜160℃、好ましくは90〜150℃の範囲で、延
伸倍率はそれぞれ3.0〜5.0倍、好ましくは3.2〜4.5倍の
範囲が好適である。また、延伸速度は1×103〜7×104
%/分の範囲が好ましい。
In the case of the sequential biaxial stretching method, it is general to stretch in the longitudinal direction and then in the width direction, but the stretching may be performed in the reverse order. The conditions for biaxial stretching are not necessarily constant depending on the stretching method, the type of polymer, etc., but are usually 80 to 160 ° C in both the longitudinal and width directions, preferably 90 to 150 ° C, and the stretching ratio is 3.0 to 5.0, respectively. A range of 2 times, preferably 3.2 to 4.5 times is suitable. The stretching speed is 1 × 10 3 to 7 × 10 4.
% / Min is preferred.

ここで、延伸する前に未延伸フィルムを100〜170℃
で、0.1〜60秒間熱処理することは、本発明のラマンバ
ンド半価幅を満足させるのに有効である。
Here, the unstretched film is stretched to 100 to 170 ° C. before stretching.
Then, the heat treatment for 0.1 to 60 seconds is effective for satisfying the Raman band half width of the present invention.

次にこの延伸フィルムを熱処理するが、この時の熱処
理条件としては、水蒸気などの雰囲気下で、130〜210
℃、特に130〜180℃の温度範囲での熱処理、またはマイ
クロ波による加熱処理が本発明のラマンバンド幅を満足
させるのに極めて有効である。時間は、0.5〜60秒間、
定長下での処理が好適である。
Next, this stretched film is heat treated. The heat treatment conditions at this time are 130 to 210 in an atmosphere such as steam.
The heat treatment in the temperature range of 130 ° C., particularly in the range of 130 to 180 ° C., or the heat treatment by microwaves is extremely effective for satisfying the Raman bandwidth of the present invention. Time is 0.5-60 seconds,
Processing under a fixed length is preferable.

[作用] 本発明は、特殊な方法によって検出されるフィルム極
表層のラマンバンド半価幅とフィルム内部の半価幅の関
係、すなわちフィルム極表層の密度とフィルム内部の密
度の関係を特定範囲としたので、フィルム表面に外から
の剪断力が加わった時の衝撃吸収力の大きいフィルムと
できた結果、本発明の効果が得られたものと推定され
る。
[Operation] In the present invention, the relationship between the Raman band half-value width of the film pole surface layer and the half-value width inside the film detected by a special method, that is, the relation between the density of the film pole surface layer and the density inside the film is set within a specific range. Therefore, it is presumed that the effect of the present invention was obtained as a result of being able to obtain a film having a large impact absorption force when an external shearing force is applied to the film surface.

[物性の測定方法ならびに効果の評価方法] 本発明の特性値の測定方法並びに効果の評価方法は次
の通りである。
[Physical property measuring method and effect evaluating method] The characteristic value measuring method and effect evaluating method of the present invention are as follows.

(1) 無機微粒子の平均粒径 フィルムからポリエステルをブラズマ灰化処理法ある
いはo−クロルフェノール溶解法で除去し、これをエタ
ノールに分散させ、遠心沈降法(堀場製作所、CAPA500
使用)で測定した体積平均径である。
(1) Average particle size of inorganic fine particles Polyester was removed from the film by a plasma ashing method or an o-chlorophenol dissolution method, and this was dispersed in ethanol, followed by centrifugal sedimentation (Horiba, CAPA500).
It is the volume average diameter measured in (use).

(2) 無機微粒子の含有量 ポリエステル100gにo−クロルフェノール1.0を加
え120℃で3時間加熱した後、日立工機(株)製超遠心
機55P−72を用い、30,000rpmで40分間延伸分離を行な
い、得られた粒子を100℃で真空乾燥する。微粒子を走
査型差動熱量計にて測定した時、ポリマに相当する融解
ピークが認められる場合には微粒子にo−クロルフェノ
ールを加熱冷却後再び延伸分離操作を行なう。融解ピー
クが認められなくなった時、微粒子を析出粒子とする。
通常延伸分離操作は2回で足りる。
(2) Content of inorganic fine particles After adding o-chlorophenol 1.0 to 100 g of polyester and heating at 120 ° C. for 3 hours, ultracentrifuge 55P-72 manufactured by Hitachi Koki Co., Ltd. was used to stretch and separate for 40 minutes at 30,000 rpm. Then, the obtained particles are vacuum dried at 100 ° C. When the melting peak corresponding to the polymer is observed when the fine particles are measured by a scanning differential calorimeter, o-chlorophenol is heated and cooled on the fine particles, and then the stretching separation operation is performed again. When no melting peak is observed, the fine particles are regarded as precipitated particles.
Usually, two stretching separation operations are sufficient.

(3) フィルム極表層ラマンバンド半価幅 Jobin−Yvon社製Ramanor U−1000ラマンシステムによ
り、全反射ラマンスペクトルを測定し、カルボニル基の
伸縮振動である1730cm-1の半価幅を求めた。測定条件は
次の通りである。測定深さは、表面から500〜1000Å。
(3) Full width half maximum Raman band of film outermost layer Ramanor U-1000 Raman system manufactured by Jobin-Yvon was used to measure the total reflection Raman spectrum, and the half width at 1730 cm -1 which is the stretching vibration of the carbonyl group was determined. The measurement conditions are as follows. The measurement depth is 500 to 1000Å from the surface.

光源 アルゴンイオンレーザー(5145Å) 試料のセッティング レーザー偏向方向(S偏向)とフィルム長手方向が平
行となるようにフィルム表面を全反射プリズムに圧着さ
せ、レーザのプリズムへの入射角(フィルム厚さ方向と
の角度)は60゜とした。
Light source Argon ion laser (5145Å) Setting the sample Press the film surface to the total reflection prism so that the laser deflection direction (S deflection) and the film longitudinal direction are parallel, and the incident angle of the laser to the prism (with the film thickness direction Angle) was set to 60 °.

検出器 PM:RCA31034/Proton Counting S ystem (Hamamatsu c1230)(SUPPLY 1600V) 測定条件 SLIT 1000μm LASER 100mW GATE TIME 1.0sec SCAN SPEED 12cm-1/min SAMPLING INTERVAL 0.2cm-1 REPEAT TIME 6 (4) フィルム内部(バルク)ラマンバンド半価幅 上記(3)と同じラマンシステムを用いた。ただし、
全反射プリズムを使用せず、またレーザーの入射角を70
゜とすることにより、正反射光は逃がし、ラマン散乱光
のみを検出した。すなわち、上記(3)の測定は光が全
反射する時にわずかにフィルム表面にしみこむことを利
用し、極表層の情報を得ているのに対し、ここでは、全
反射をさせないでフィルム内部のラマン散乱光からの情
報を得ているものである。その他の条件は、REPEAT・TI
MEが4回である以外は上記(3)と同じである。
Detector PM: RCA31034 / Proton Counting System (Hamamatsu c1230) (SUPPLY 1600V) Measuring condition SLIT 1000μm LASER 100mW GATE TIME 1.0sec SCAN SPEED 12cm -1 / min SAMPLING INTERVAL 0.2cm -1 REPEAT TIME 6 (4) Inside film ( (Bulk) Raman band half width The same Raman system as in (3) above was used. However,
Without using a total reflection prism, the laser incident angle is 70
By setting the angle to be °, the specularly reflected light escaped, and only the Raman scattered light was detected. That is, in the measurement of the above (3), the information on the extreme surface layer is obtained by utilizing the fact that the light slightly penetrates into the film surface when the light is totally reflected, whereas the Raman inside the film is obtained without total reflection here. The information is obtained from the scattered light. Other conditions are REPEAT / TI
Same as (3) above except that ME is 4 times.

(5) 面配向指数 ナトリウムD線(波長589nm)を光源としてアツベ屈
折率計を用いて、二軸配向フィルムの厚さ方向の屈折率
(Aとする)および溶融プレス後10℃の水中へ急冷して
作った無配向(アモルファス)フィルムの厚さ方向の屈
折率(Bとする)を測定し、A/Bをもって面配向指数と
した。マウント液にはヨウ化メチレンを用い、25℃、65
%RHにて測定した。
(5) Plane orientation index Using an Abebe refractometer with sodium D line (wavelength 589 nm) as a light source, the biaxially oriented film has a refractive index (A) in the thickness direction and is rapidly cooled into water at 10 ° C. after melt pressing. The refractive index (denoted as B) in the thickness direction of the non-oriented (amorphous) film thus prepared was measured, and A / B was taken as the plane orientation index. Use methylene iodide as the mounting solution at 25 ° C and 65
It was measured at% RH.

(6) 溶融粘度 高化式フローテスターを用いて、温度290℃、ずり速
度200sec-1で測定した。
(6) Melt viscosity The melt viscosity was measured using a high flow tester at a temperature of 290 ° C. and a shear rate of 200 sec −1 .

(7) 表面平均粗さRa 触針式表面粗さ計を用い、JIS−B−0601にしたがっ
て測定した。ただし、カットオフは0.08mm、測定長は1m
mとした。
(7) Surface average roughness Ra was measured according to JIS-B-0601 using a stylus type surface roughness meter. However, the cutoff is 0.08 mm, and the measurement length is 1 m.
It was m.

(8) ガラス転移点Tg、冷結晶化温度Tcc パーキンエルマー社製のDSC(示差走査熱量計)II型
を用いて測定した。DSCの測定条件は次の通りである。
すなわち、試料10mgをDSC装置にセットし、300℃の温度
で5分間溶融した後、液体窒素中に急冷する。この急冷
試料を10℃/分で昇温し、ガラス転移点Tgを検知する。
さらに昇温を続け、ガラス状態からの結晶化発熱ピーク
温度をもって冷結晶化温度Tccとした。ここでTccとTgの
差(Tcc−Tg)を△Tcgと定義する。
(8) Glass transition point Tg, cold crystallization temperature Tcc It was measured using a Perkin-Elmer DSC (differential scanning calorimeter) type II. The DSC measurement conditions are as follows.
That is, 10 mg of a sample is set in a DSC apparatus, melted at a temperature of 300 ° C. for 5 minutes, and then rapidly cooled in liquid nitrogen. The temperature of this quenched sample is raised at 10 ° C./min, and the glass transition point Tg is detected.
The temperature was further raised, and the crystallization exothermic peak temperature from the glass state was set as the cold crystallization temperature Tcc. Here, the difference between Tcc and Tg (Tcc-Tg) is defined as ΔTcg.

(9) 結晶化促進係数(単位は℃) 上記方法で1重量%の不活性無機粒子を含有するポリ
エステルの△Tcg(I)、およびこれと同粘度の不活性
無機粒子を含有しないポリエステルの△Tcg(II)を測
定し、△Tcg(II)と△Tcg(I)の差[△Tcg(II)−
△Tcg(I)]をもって、その不活性無機粒子の結晶化
促進係数とした。
(9) Crystallization acceleration coefficient (unit: ° C.) ΔTcg (I) of the polyester containing 1% by weight of the inert inorganic particles by the above method, and ΔTcg (I) of the polyester containing no inert inorganic particles of the same viscosity. Tcg (II) is measured and the difference between ΔTcg (II) and ΔTcg (I) [ΔTcg (II)-
ΔTcg (I)] was used as the crystallization promoting coefficient of the inert inorganic particles.

(10) 耐削れ性 フィルムを幅1/2インチにテープ状にスリットしたも
のに片刃を垂直に押しあて、さらに0.5mm押し込んだ状
態で20cm走行させる(走行張力500g、走行速度6.7cm/
秒)。この時、片刃の先に付着したフィルム表面の削れ
物の高さを顕微鏡で読みとり、削れ量とした(単位はμ
m)。この削れ量(両面の平均値)が15μm以下の場合
は耐削れ性:良好、15μmを越える場合は耐削れ性:不
良と判定した。この削れ量:15μmという値は、印刷工
程やカレンダー工程などの加工工程で、フィルム表面が
削れることによって、工程上、製品性能上のトラブルが
起るか否かの臨界点である。
(10) Scraping resistance A film is slit into a tape with a width of 1/2 inch, a single blade is pressed vertically, and the product is run for 20 cm while being pushed 0.5 mm (running tension 500 g, running speed 6.7 cm /
Seconds). At this time, the height of the shavings on the surface of the film attached to the tip of the single blade was read with a microscope and used as the shaving amount (unit: μ
m). When the abrasion amount (average value on both surfaces) was 15 μm or less, abrasion resistance was good, and when it was more than 15 μm, abrasion resistance was judged to be poor. The scraped amount: 15 μm is a critical point whether or not a process surface or product performance trouble occurs due to scraping of the film surface in a processing step such as a printing step or a calendar step.

[実施例] 本発明を実施例に基づいて説明する。[Examples] The present invention will be described based on Examples.

実施例1 平均粒径0.3μmの酸化チタンを濃度1重量%でエチ
レングリコールにスラリーの形で分散させた。この時、
酸化チタンに対し、1重量%のテトラエチルアンモニウ
ムリン酸塩(リン酸とテトラエチルアンモニウムハイド
ロオキサイドをモル比1:1で混合)を添加し、50μm径
のガラスビースをメディアとして分散させたのち、ガラ
スビースを過して除いてスラリーを調製した。このエ
チレングリコールとテレフタル酸ジメチルをエステル交
換反応後重縮合して、酸化チタン粒子を1重量%含有す
るポリエチレンテレフタレートを作った。この酸化チタ
ンの結晶化促進係数は2.5℃であった。
Example 1 Titanium oxide having an average particle size of 0.3 μm was dispersed in ethylene glycol in a slurry form at a concentration of 1% by weight. This time,
To titanium oxide, 1% by weight of tetraethylammonium phosphate (phosphoric acid and tetraethylammonium hydroxide were mixed at a molar ratio of 1: 1) was added, and glass beads having a diameter of 50 μm were dispersed as a medium. Was removed to prepare a slurry. This ethylene glycol and dimethyl terephthalate were transesterified and then polycondensed to produce polyethylene terephthalate containing 1% by weight of titanium oxide particles. The crystallization acceleration coefficient of this titanium oxide was 2.5 ° C.

このポリエチレンテレフタレートのペレットと無機粒
子を含有しないポリエチレンテレフタレートのペレット
とを、酸化チタン含有量が0.4重量%となるように混合
した。この混合ペレットを180℃で3時間減圧乾燥(3To
rr)した。このペレットを押出機に供給し、300℃で溶
融押出し、ドラフト比を15として、静電印加キャスト法
を用いて表面温度を30℃のキャスティング・ドラムに巻
きつけて冷却固化し、厚さ約180μmの未延伸フィルム
を作った。この未延伸フィルムを130℃で1分間熱処理
したのち、90℃にて長手方向に3.4倍延伸した。
The polyethylene terephthalate pellets and the polyethylene terephthalate pellets containing no inorganic particles were mixed so that the titanium oxide content was 0.4% by weight. This mixed pellet was dried under reduced pressure at 180 ° C for 3 hours (3To
rr) did. These pellets are supplied to an extruder, melt-extruded at 300 ° C, the draft ratio is set to 15, and the surface temperature is wrapped around a casting drum at a surface temperature of 30 ° C by using the electrostatically applied casting method to cool and solidify, and the thickness is about 180 μm. Of unstretched film. This unstretched film was heat-treated at 130 ° C. for 1 minute and then stretched at 90 ° C. in the longitudinal direction by a factor of 3.4.

この延伸は2組のロールの周速差で行なわれ、延伸速
度10000%/分であった。この一軸フィルムをステンタ
を用いて延伸速度2000%/分で100℃で軸方向に3.6倍延
伸した。このフィルムを水蒸気中で、140℃で20秒間熱
処理して厚さ15μmの二軸配向フィルムを得た。このフ
ィルムの極表層のラマンバンド半価幅は両面とも18c
m-1、フィルム内部のラマンバンド半価幅は16cm-1と、
その差は2cm-1であり本発明の関係を満足するものであ
った。このフィルムの表面の削れ性を調べた結果、削れ
量は4μmであり、耐削れ性は良好であった。
This drawing was carried out at a peripheral speed difference between the two sets of rolls, and the drawing speed was 10,000% / min. This uniaxial film was stretched 3.6 times in the axial direction at 100 ° C. at a stretching rate of 2000% / min using a stenter. This film was heat-treated in steam at 140 ° C. for 20 seconds to obtain a biaxially oriented film having a thickness of 15 μm. The Raman band half width of the extreme surface layer of this film is 18c on both sides.
m -1 , the Raman band half width at the inside of the film is 16 cm -1 ,
The difference was 2 cm -1 , which satisfied the relationship of the present invention. As a result of examining the abrasion resistance of the surface of this film, the abrasion amount was 4 μm and the abrasion resistance was good.

実施例2〜4、比較例1〜3 平均粒径0.5μmの各種無機粒子を分散方法を種々変
更してエチレングリコールにスラリーの形で分散させた
(無機粒子の濃度は1重量%)。このエチレングリコー
ルとテレフタル酸ジメチルをエステル交換反応後重縮合
して、無機粒子を1重量%含有するポリエチレンテレフ
タレートを作った。これらの無機粒子の結晶化促進係数
は第1表に示したとおりであった。
Examples 2 to 4 and Comparative Examples 1 to 3 Various inorganic particles having an average particle diameter of 0.5 μm were dispersed in ethylene glycol in the form of a slurry by changing the dispersion method (the concentration of the inorganic particles was 1% by weight). This ethylene glycol and dimethyl terephthalate were transesterified and then polycondensed to produce polyethylene terephthalate containing 1% by weight of inorganic particles. The crystallization acceleration coefficient of these inorganic particles was as shown in Table 1.

これらのポリエチレンテレフタレートのペレットと無
機粒子を含有しないポリエチレンテレフタレートのペレ
ットを無機粒子含有量が0.25重量%となるように混合し
た。この混合ペレットを180℃で3時間減圧乾燥(3Tor
r)した。このペレットを押出機に供給し、300℃で溶融
押出し、ドラフト比を15として、静電印加キャスト法を
用いて表面温度30℃のキャスティング・ドラムに巻きつ
けて冷却固化し、厚さ約180μmの未延伸フィルムを作
った。この未延伸フィルムを各種処理をしたのち、90℃
にて長手方向に3.4倍延伸した。
These polyethylene terephthalate pellets and polyethylene terephthalate pellets containing no inorganic particles were mixed so that the content of inorganic particles was 0.25% by weight. This mixed pellet was dried under reduced pressure at 180 ° C for 3 hours (3 Tor
r) done. These pellets were fed to an extruder, melt-extruded at 300 ° C, and the draft ratio was set to 15. The pellet was wound around a casting drum with a surface temperature of 30 ° C using an electrostatic cast method to be cooled and solidified to a thickness of about 180 μm. An unstretched film was made. After various processing of this unstretched film, 90 ℃
Was stretched 3.4 times in the longitudinal direction.

この延伸は2組のロールの周速差で行なわれ、延伸速
度10000%/分であった。この一軸フィルムをステンタ
を用いて延伸速度2000%/分で100℃で幅方向に3.6倍延
伸した。このフィルムを各種方法にて10秒間熱処理して
厚さ15μmのフィルムを得た。
This drawing was carried out at a peripheral speed difference between the two sets of rolls, and the drawing speed was 10,000% / min. This uniaxial film was stretched 3.6 times in the width direction at 100 ° C. at a stretching rate of 2000% / min using a stenter. This film was heat-treated for 10 seconds by various methods to obtain a film having a thickness of 15 μm.

これらのフィルムの極表層のラマンバンド半価幅、フ
ィルム内部のラマンバンド半価幅、フィルムの耐削れ性
は第1表に示したとおりであり、ラマンバンド半価幅が
本発明範囲内の場合は耐削れ性が良好であったが、そう
でない場合は不良であった。不活性無機粒子の種類は同
じでも、そのフィルムのラマンバンド半価幅の関係によ
り、耐削れ性が大きく異なることがわかる。
The Raman band full width at half maximum of these films, the Raman band half width at the inside of the film, and the abrasion resistance of the film are as shown in Table 1. When the Raman band half width is within the range of the present invention Had good abrasion resistance, but otherwise it was poor. It can be seen that even if the types of the inert inorganic particles are the same, the abrasion resistance greatly differs depending on the Raman band half-value width relationship of the film.

[発明の効果] 本発明は、特殊な方法によって検出されるフィルム極
表層のラマンバンド半価幅とフィルム内部の半価幅の関
係、すなわち、フィルム極表層の密度と内部の密度の関
係をコントロールできた結果、表面の耐削れ性を向上さ
せることができ、加工工程が高速化されても、加工工程
上、製品性能上のトラブルの原因となるフィルム表面の
削れが起らないフィルムが得られたものである。
EFFECTS OF THE INVENTION The present invention controls the relationship between the Raman band half-value width of the film polar surface layer and the half-value width inside the film, that is, the relationship between the density of the film polar surface layer and the internal density, which is detected by a special method. As a result, the abrasion resistance of the surface can be improved, and even if the processing speed is increased, it is possible to obtain a film in which the surface of the film is not scraped, which causes troubles in the product performance in the processing process. It is a thing.

本発明フィルムの用途は特に限定されないが、フィル
ムの削れが製品性能のトラブルとなるやすい磁気記録媒
体、特にビデオテープ用ベースフィルムとして有用であ
る。
The use of the film of the present invention is not particularly limited, but the film of the present invention is useful as a base film for a magnetic recording medium, particularly a video tape, in which abrasion of the film tends to cause troubles in product performance.

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 C08L 67:02 ─────────────────────────────────────────────────── ─── Continuation of the front page (51) Int.Cl. 6 Identification code Internal reference number FI technical display area C08L 67:02

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】ポリエステルと、少なくとも一種類の不活
性無機粒子からなる組成物を主たる成分とする二軸配向
フィルムであって、少なくとも片面のフィルムの極表層
(フィルム表面からの深さ1000Åまでの部分)のカルボ
ニル基によるラマンバンドの半価幅が、フィルム内部
(該フィルム極表層以外の部分)の半価幅より1cm-1
上大きいことを特徴とする二軸配向ポリエステルフィル
ム。
1. A biaxially oriented film comprising a polyester and a composition comprising at least one kind of inert inorganic particles as a main component, wherein the film has at least one extreme surface layer (a depth from the surface of the film of up to 1000 Å). The biaxially oriented polyester film is characterized in that the half-value width of the Raman band due to the carbonyl group of (part) is larger than the half-value width inside the film (the part other than the film outermost layer) by 1 cm -1 or more.
JP62054584A 1987-03-10 1987-03-10 Polyester film Expired - Fee Related JPH089670B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62054584A JPH089670B2 (en) 1987-03-10 1987-03-10 Polyester film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62054584A JPH089670B2 (en) 1987-03-10 1987-03-10 Polyester film

Publications (2)

Publication Number Publication Date
JPS63221136A JPS63221136A (en) 1988-09-14
JPH089670B2 true JPH089670B2 (en) 1996-01-31

Family

ID=12974754

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62054584A Expired - Fee Related JPH089670B2 (en) 1987-03-10 1987-03-10 Polyester film

Country Status (1)

Country Link
JP (1) JPH089670B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5320920B2 (en) * 2008-09-16 2013-10-23 東レ株式会社 Polyester film

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0756689B2 (en) * 1984-09-12 1995-06-14 帝人株式会社 Biaxially stretched polyester film
JPS61254328A (en) * 1985-05-08 1986-11-12 Teijin Ltd Biaxially oriented polyester film for magnetic recording

Also Published As

Publication number Publication date
JPS63221136A (en) 1988-09-14

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